Deprecated: $wgMWOAuthSharedUserIDs=false is deprecated, set $wgMWOAuthSharedUserIDs=true, $wgMWOAuthSharedUserSource='local' instead [Called from MediaWiki\HookContainer\HookContainer::run in /var/www/html/w/includes/HookContainer/HookContainer.php at line 135] in /var/www/html/w/includes/Debug/MWDebug.php on line 372
On asymptotic formulae for solutions to differential equations with summable coefficients - MaRDI portal

On asymptotic formulae for solutions to differential equations with summable coefficients (Q2711768)

From MaRDI portal





scientific article
Language Label Description Also known as
English
On asymptotic formulae for solutions to differential equations with summable coefficients
scientific article

    Statements

    0 references
    0 references
    25 April 2001
    0 references
    linear system
    0 references
    \(L\)-diagonal system
    0 references
    small parameter
    0 references
    asymptotic expansion
    0 references
    On asymptotic formulae for solutions to differential equations with summable coefficients (English)
    0 references
    The authors suggest a method for the construction of asymptotic solutions to the linear system \(\dot x=A(t)x\) by reducing it to the so-called \(L\)-diagonal form. It is assumed that on \([t_0,\infty)\) the eigenvalues of matrix \(A(t)\) are multiple, the corresponding elementary divisors are of constant multiplicity, and the matrix \(D(t):=J(t)+T^{-1}(t)T'(t)\) has simple eigenvalues. Here, \(J(t)\) is the Jordan normal form of \(A(t)\) and \(T(t)\) is such a nonsingular matrix that \(T^{-1}(t)A(t)(t)T(t)=J(t)\). Thus after the change of variables \(x=T(t)y\) one obtains a system of the form \(\dot y=D(t)y\). By introducing an artificial small parameter \(\varepsilon \) the authors apply a method of asymptotic diagonalization to the system NEWLINE\[NEWLINE\varepsilon \dot y=D(t)y.\tag{1}NEWLINE\]NEWLINE More precisely, the matrix \(U_m(t, \varepsilon)=\sum_{s=0}^{m}\varepsilon^sU_s(t)\) is constructed in such a way that the change of variables \(y=U_m(t,\varepsilon)z\) transforms (1) to the system NEWLINE\[NEWLINE\varepsilon \dot z=(\Lambda_m(t,\varepsilon)+\varepsilon ^{m+1}C_ m(t,\varepsilon))z\tag{2}NEWLINE\]NEWLINE with the diagonal matrix \(\Lambda_m(t,\varepsilon) \sum_{s=0}^{m}\varepsilon^s\Lambda_s(t)\). Under the assumptions that for \(\varepsilon =1\) the eigenvalues of this matrix have different real parts on \([ t_0,\infty)\) and \(\int_{t_0}^{\infty }\|C_m(t,1)\|dt<\infty \), the authors apply well known results from the theory of \(L\)-diagonal systems [see, e.g. \textit{R. Bellman}, Stability theory of differential equations. New York-London: McGraw-Hill Book Company (1953; Zbl 0053.24705)] to construct solutions to system (1) for \(\varepsilon =1\).NEWLINENEWLINEFor the entire collection see [Zbl 0937.00046].
    0 references

    Identifiers

    0 references
    0 references
    0 references
    0 references